New Perspectives on Polyhedral Molecules and Their Crystal Structures Santiago Alvarez, Jorge Echeverria
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Symmetry of Fulleroids Stanislav Jendrol’, František Kardoš
Symmetry of Fulleroids Stanislav Jendrol’, František Kardoš To cite this version: Stanislav Jendrol’, František Kardoš. Symmetry of Fulleroids. Klaus D. Sattler. Handbook of Nanophysics: Clusters and Fullerenes, CRC Press, pp.28-1 - 28-13, 2010, 9781420075557. hal- 00966781 HAL Id: hal-00966781 https://hal.archives-ouvertes.fr/hal-00966781 Submitted on 27 Mar 2014 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Symmetry of Fulleroids Stanislav Jendrol’ and Frantiˇsek Kardoˇs Institute of Mathematics, Faculty of Science, P. J. Saf´arikˇ University, Koˇsice Jesenn´a5, 041 54 Koˇsice, Slovakia +421 908 175 621; +421 904 321 185 [email protected]; [email protected] Contents 1 Symmetry of Fulleroids 2 1.1 Convexpolyhedraandplanargraphs . .... 3 1.2 Polyhedral symmetries and graph automorphisms . ........ 4 1.3 Pointsymmetrygroups. 5 1.4 Localrestrictions ............................... .. 10 1.5 Symmetryoffullerenes . .. 11 1.6 Icosahedralfulleroids . .... 12 1.7 Subgroups of Ih ................................. 15 1.8 Fulleroids with multi-pentagonal faces . ......... 16 1.9 Fulleroids with octahedral, prismatic, or pyramidal symmetry ........ 19 1.10 (5, 7)-fulleroids .................................. 20 1 Chapter 1 Symmetry of Fulleroids One of the important features of the structure of molecules is the presence of symmetry elements. -
Origin of Icosahedral Symmetry in Viruses
Origin of icosahedral symmetry in viruses Roya Zandi†‡, David Reguera†, Robijn F. Bruinsma§, William M. Gelbart†, and Joseph Rudnick§ Departments of †Chemistry and Biochemistry and §Physics and Astronomy, University of California, Los Angeles, CA 90095-1569 Communicated by Howard Reiss, University of California, Los Angeles, CA, August 11, 2004 (received for review February 2, 2004) With few exceptions, the shells (capsids) of sphere-like viruses (11). This problem is in turn related to one posed much earlier have the symmetry of an icosahedron and are composed of coat by Thomson (12), involving the optimal distribution of N proteins (subunits) assembled in special motifs, the T-number mutually repelling points on the surface of a sphere, and to the structures. Although the synthesis of artificial protein cages is a subsequently posed ‘‘covering’’ problem, where one deter- rapidly developing area of materials science, the design criteria for mines the arrangement of N overlapping disks of minimum self-assembled shells that can reproduce the remarkable properties diameter that allow complete coverage of the sphere surface of viral capsids are only beginning to be understood. We present (13). In a similar spirit, a self-assembly phase diagram has been here a minimal model for equilibrium capsid structure, introducing formulated for adhering hard disks (14). These models, which an explicit interaction between protein multimers (capsomers). all deal with identical capsomers, regularly produced capsid Using Monte Carlo simulation we show that the model reproduces symmetries lower than icosahedral. On the other hand, theo- the main structures of viruses in vivo (T-number icosahedra) and retical studies of viral assembly that assume icosahedral sym- important nonicosahedral structures (with octahedral and cubic metry are able to reproduce the CK motifs (15), and, most symmetry) observed in vitro. -
Mass Spectrometric Research of Hydrogenated Molecules of Carbon As Products of Pyrolysis of Benzene and Pyridine Vapours
Chemical and Materials Engineering 1(4): 122-131, 2013 http://www.hrpub.org DOI: 10.13189/cme.2013.010404 Mass Spectrometric Research of Hydrogenated Molecules of Carbon as Products of Pyrolysis of Benzene and Pyridine Vapours Alexey Kharlamov1, Marina Bondarenko1,*, Ganna Kharlamova2 1Frantsevich Institute for Problems of Materials Science of NASU, Krzhyzhanovsky St. 3, 03680 Kiev, Ukraine 2Taras Shevchenko National University of Kiev, Volodymyrs'ka St. 64, 01601 Kiev, Ukraine *Corresponding Author: [email protected] Copyright © 2013 Horizon Research Publishing All rights reserved. Abstract Hydrogenated carbon molecules are to speak about creation on the basis of system of convertible synthesized by a method which essentially is distinct from reactions already known methods of preparation of fulleranes as this C60+30H2 C60H60 (1) method a preliminary stage of synthesis of carbon molecules accumulator of hydrogen with so huge (7.7mass. %) contents is excluded completely. Fulleranes and quasi-fulleranes as ⇌ of hydrogen. Though here it is necessary to note, that in nanodimentional particles were in common deposited by dodecahedrane С Н , which was synthesized by Paquette ethanol from benzene-xylene extracts from products of 20 20 [4] three years prior to opening of fullerene С (and 8 years pyrolysis of vapours of benzene and pyridine. The 60 prior to obtaining of first fullerane C H ), the ratio Н/C is dehydrogenation of the synthesized samples of fulleranes 60 36 the same (1/12) as in fullerene С Н . However of so and quasi-fulleranes is started at 30-50 °C and the evacuation 60 60 steadfast interest of the researchers this controllable of hydrogen proceeds up to 700 °C. -
E8 Physics and Quasicrystals Icosidodecahedron and Rhombic Triacontahedron Vixra 1301.0150 Frank Dodd (Tony) Smith Jr
E8 Physics and Quasicrystals Icosidodecahedron and Rhombic Triacontahedron vixra 1301.0150 Frank Dodd (Tony) Smith Jr. - 2013 The E8 Physics Model (viXra 1108.0027) is based on the Lie Algebra E8. 240 E8 vertices = 112 D8 vertices + 128 D8 half-spinors where D8 is the bivector Lie Algebra of the Real Clifford Algebra Cl(16) = Cl(8)xCl(8). 112 D8 vertices = (24 D4 + 24 D4) = 48 vertices from the D4xD4 subalgebra of D8 plus 64 = 8x8 vertices from the coset space D8 / D4xD4. 128 D8 half-spinor vertices = 64 ++half-half-spinors + 64 --half-half-spinors. An 8-dim Octonionic Spacetime comes from the Cl(8) factors of Cl(16) and a 4+4 = 8-dim Kaluza-Klein M4 x CP2 Spacetime emerges due to the freezing out of a preferred Quaternionic Subspace. Interpreting World-Lines as Strings leads to 26-dim Bosonic String Theory in which 10 dimensions reduce to 4-dim CP2 and a 6-dim Conformal Spacetime from which 4-dim M4 Physical Spacetime emerges. Although the high-dimensional E8 structures are fundamental to the E8 Physics Model it may be useful to see the structures from the point of view of the familiar 3-dim Space where we live. To do that, start by looking the the E8 Root Vector lattice. Algebraically, an E8 lattice corresponds to an Octonion Integral Domain. There are 7 Independent E8 Lattice Octonion Integral Domains corresponding to the 7 Octonion Imaginaries, as described by H. S. M. Coxeter in "Integral Cayley Numbers" (Duke Math. J. 13 (1946) 561-578 and in "Regular and Semi-Regular Polytopes III" (Math. -
Archimedean Solids
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln MAT Exam Expository Papers Math in the Middle Institute Partnership 7-2008 Archimedean Solids Anna Anderson University of Nebraska-Lincoln Follow this and additional works at: https://digitalcommons.unl.edu/mathmidexppap Part of the Science and Mathematics Education Commons Anderson, Anna, "Archimedean Solids" (2008). MAT Exam Expository Papers. 4. https://digitalcommons.unl.edu/mathmidexppap/4 This Article is brought to you for free and open access by the Math in the Middle Institute Partnership at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in MAT Exam Expository Papers by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. Archimedean Solids Anna Anderson In partial fulfillment of the requirements for the Master of Arts in Teaching with a Specialization in the Teaching of Middle Level Mathematics in the Department of Mathematics. Jim Lewis, Advisor July 2008 2 Archimedean Solids A polygon is a simple, closed, planar figure with sides formed by joining line segments, where each line segment intersects exactly two others. If all of the sides have the same length and all of the angles are congruent, the polygon is called regular. The sum of the angles of a regular polygon with n sides, where n is 3 or more, is 180° x (n – 2) degrees. If a regular polygon were connected with other regular polygons in three dimensional space, a polyhedron could be created. In geometry, a polyhedron is a three- dimensional solid which consists of a collection of polygons joined at their edges. The word polyhedron is derived from the Greek word poly (many) and the Indo-European term hedron (seat). -
Functionalized Aromatics Aligned with the Three Cartesian Axes: Extension of Centropolyindane Chemistry*
Pure Appl. Chem., Vol. 78, No. 4, pp. 749–775, 2006. doi:10.1351/pac200678040749 © 2006 IUPAC Functionalized aromatics aligned with the three Cartesian axes: Extension of centropolyindane chemistry* Dietmar Kuck‡ Fakultät für Chemie, Universität Bielefeld, Universitätsstraße 25, D-33615 Bielefeld, Germany Abstract: The unique geometrical features and structural potential of the centropolyindanes, a complete family of novel, 3D polycyclic aromatic hydrocarbons, are discussed with respect to the inherent orthogonality of their arene units. Thus, the largest member of the family, centrohexaindane, a topologically nonplanar hydrocarbon, is presented as a “Cartesian hexa- benzene”, because each of its six benzene units is stretched into one of the six directions of the Cartesian space. This feature is discussed on the basis of the X-ray crystal structures of centrohexaindane and two lower members of the centropolyindane family, viz. the parent tribenzotriquinacenes. Recent progress in multiple functionalization and extension of the in- dane wings of selected centropolyindanes is reported, including several highly efficient six- and eight-fold C–C cross-coupling reactions. Some particular centropolyindane derivatives are presented, such as the first twelve-fold functionalized centrohexaindane and a tribenzo- triquinacene bearing three mutually orthogonal phenanthroline groupings at its molecular pe- riphery. Challenges to further extend the arene peripheries of the tribenzotriquinacenes and fenestrindanes to give, eventually, graphite cuttings bearing a central bowl- or saddle-shaped center are outlined, as is the hypothetical generation of a “giant” nanocube consisting of eight covalently bound tribenzotriquinacene units. Along these lines, our recent discovery of a re- lated, solid-state supramolecular cube, containing eight molecules of a particular tri- bromotrinitrotribenzotriquinacene of the same absolute configuration, is presented for the first time. -
The Cubic Groups
The Cubic Groups Baccalaureate Thesis in Electrical Engineering Author: Supervisor: Sana Zunic Dr. Wolfgang Herfort 0627758 Vienna University of Technology May 13, 2010 Contents 1 Concepts from Algebra 4 1.1 Groups . 4 1.2 Subgroups . 4 1.3 Actions . 5 2 Concepts from Crystallography 6 2.1 Space Groups and their Classification . 6 2.2 Motions in R3 ............................. 8 2.3 Cubic Lattices . 9 2.4 Space Groups with a Cubic Lattice . 10 3 The Octahedral Symmetry Groups 11 3.1 The Elements of O and Oh ..................... 11 3.2 A Presentation of Oh ......................... 14 3.3 The Subgroups of Oh ......................... 14 2 Abstract After introducing basics from (mathematical) crystallography we turn to the description of the octahedral symmetry groups { the symmetry group(s) of a cube. Preface The intention of this account is to provide a description of the octahedral sym- metry groups { symmetry group(s) of the cube. We first give the basic idea (without proofs) of mathematical crystallography, namely that the 219 space groups correspond to the 7 crystal systems. After this we come to describing cubic lattices { such ones that are built from \cubic cells". Finally, among the cubic lattices, we discuss briefly the ones on which O and Oh act. After this we provide lists of the elements and the subgroups of Oh. A presentation of Oh in terms of generators and relations { using the Dynkin diagram B3 is also given. It is our hope that this account is accessible to both { the mathematician and the engineer. The picture on the title page reflects Ha¨uy'sidea of crystal structure [4]. -
Volume Estimates for Equiangular Hyperbolic Coxeter Polyhedra
Algebraic & Geometric Topology 9 (2009) 1225–1254 1225 Volume estimates for equiangular hyperbolic Coxeter polyhedra CHRISTOPHER KATKINSON An equiangular hyperbolic Coxeter polyhedron is a hyperbolic polyhedron where all dihedral angles are equal to =n for some fixed n Z, n 2. It is a consequence of 2 Andreev’s theorem that either n 3 and the polyhedron has all ideal vertices or that D n 2. Volume estimates are given for all equiangular hyperbolic Coxeter polyhedra. D 57M50; 30F40 1 Introduction An orientable 3–orbifold, Q, is determined by an underlying 3–manifold, XQ and a trivalent graph, †Q , labeled by integers. If Q carries a hyperbolic structure then it is unique by Mostow rigidity, so the hyperbolic volume of Q is an invariant of Q. Therefore, for hyperbolic orbifolds with a fixed underlying manifold, the volume is a function of the labeled graph †. In this paper, methods for estimating the volume of orbifolds of a restricted type in terms of this labeled graph will be described. The orbifolds studied in this paper are quotients of H3 by reflection groups generated by reflections in hyperbolic Coxeter polyhedra. A Coxeter polyhedron is one where each dihedral angle is of the form =n for some n Z, n 2. Given a hyperbolic 2 Coxeter polyhedron P , consider the group generated by reflections through the geodesic planes determined by its faces, .P/. Then .P/ is a Kleinian group which acts on H3 with fundamental domain P . The quotient, O H3= .P/, is a nonorientable D orbifold with singular locus P.2/ , the 2–skeleton of P . -
Construction of Great Icosidodecahedron This Paper
Construction of Great IcosiDodecahedron This paper describes how to create the Great Icosidodecahedron analytically as a 3D object. This uniform polyhedron is particularly beautiful and can be constructed with 12 pentagrams and 20 equilateral triangles. You start with a pentagon and create the net for a Icosidodecahedron without the triangles (fig 1). Extend the sides of the pentagons to create pentagrams and fold the sides into the same planes as the icosidodecahedron and you get the first half of the polyhedron (fig 2). Now for the equilateral triangles. Pick every combination of two pentagrams where a single vertex shares a common point (fig 3). Create two equilateral triangles connecting the common vertex and each of the legs of the two pentagrams. Do this to for all pentagrams and you will come up with 20 distinct intersecting triangles. The final result is in figure 4. We can create the model using a second method. Based on the geometry of the existing model, create a single cup (fig 5). Add the adjoining pentagram star (fig 6). Now take this shape and rotate- duplicate for each plane of the pentagon icosidodecahedron and you get the model of figure 4. 1 Construction of Great IcosiDodecahedron fig1 The net for the Icosidodecahedron without the triangle faces. I start with a pentagon, triangulate it with an extra point in the center. 2 Construction of Great IcosiDodecahedron fig 2 Extend the sides of the pentagons to make pentagrams then fold the net into the same planes as the Icosidodecahedron. This makes 12 intersecting stars (pentagrams). fig 3 Now add equilateral triangles to each pair of pentagrams, which touch in only one vertex. -
Can Every Face of a Polyhedron Have Many Sides ?
Can Every Face of a Polyhedron Have Many Sides ? Branko Grünbaum Dedicated to Joe Malkevitch, an old friend and colleague, who was always partial to polyhedra Abstract. The simple question of the title has many different answers, depending on the kinds of faces we are willing to consider, on the types of polyhedra we admit, and on the symmetries we require. Known results and open problems about this topic are presented. The main classes of objects considered here are the following, listed in increasing generality: Faces: convex n-gons, starshaped n-gons, simple n-gons –– for n ≥ 3. Polyhedra (in Euclidean 3-dimensional space): convex polyhedra, starshaped polyhedra, acoptic polyhedra, polyhedra with selfintersections. Symmetry properties of polyhedra P: Isohedron –– all faces of P in one orbit under the group of symmetries of P; monohedron –– all faces of P are mutually congru- ent; ekahedron –– all faces have of P the same number of sides (eka –– Sanskrit for "one"). If the number of sides is k, we shall use (k)-isohedron, (k)-monohedron, and (k)- ekahedron, as appropriate. We shall first describe the results that either can be found in the literature, or ob- tained by slight modifications of these. Then we shall show how two systematic ap- proaches can be used to obtain results that are better –– although in some cases less visu- ally attractive than the old ones. There are many possible combinations of these classes of faces, polyhedra and symmetries, but considerable reductions in their number are possible; we start with one of these, which is well known even if it is hard to give specific references for precisely the assertion of Theorem 1. -
The Truncated Icosahedron As an Inflatable Ball
https://doi.org/10.3311/PPar.12375 Creative Commons Attribution b |99 Periodica Polytechnica Architecture, 49(2), pp. 99–108, 2018 The Truncated Icosahedron as an Inflatable Ball Tibor Tarnai1, András Lengyel1* 1 Department of Structural Mechanics, Faculty of Civil Engineering, Budapest University of Technology and Economics, H-1521 Budapest, P.O.B. 91, Hungary * Corresponding author, e-mail: [email protected] Received: 09 April 2018, Accepted: 20 June 2018, Published online: 29 October 2018 Abstract In the late 1930s, an inflatable truncated icosahedral beach-ball was made such that its hexagonal faces were coloured with five different colours. This ball was an unnoticed invention. It appeared more than twenty years earlier than the first truncated icosahedral soccer ball. In connection with the colouring of this beach-ball, the present paper investigates the following problem: How many colourings of the dodecahedron with five colours exist such that all vertices of each face are coloured differently? The paper shows that four ways of colouring exist and refers to other colouring problems, pointing out a defect in the colouring of the original beach-ball. Keywords polyhedron, truncated icosahedron, compound of five tetrahedra, colouring of polyhedra, permutation, inflatable ball 1 Introduction Spherical forms play an important role in different fields – not even among the relics of the Romans who inherited of science and technology, and in different areas of every- many ball games from the Greeks. day life. For example, spherical domes are quite com- The Romans mainly used balls composed of equal mon in architecture, and spherical balls are used in most digonal panels, forming a regular hosohedron (Coxeter, 1973, ball games. -
Putting the Icosahedron Into the Octahedron
Forum Geometricorum Volume 17 (2017) 63–71. FORUM GEOM ISSN 1534-1178 Putting the Icosahedron into the Octahedron Paris Pamfilos Abstract. We compute the dimensions of a regular tetragonal pyramid, which allows a cut by a plane along a regular pentagon. In addition, we relate this construction to a simple construction of the icosahedron and make a conjecture on the impossibility to generalize such sections of regular pyramids. 1. Pentagonal sections The present discussion could be entitled Organizing calculations with Menelaos, and originates from a problem from the book of Sharygin [2, p. 147], in which it is required to construct a pentagonal section of a regular pyramid with quadrangular F J I D T L C K H E M a x A G B U V Figure 1. Pentagonal section of quadrangular pyramid basis. The basis of the pyramid is a square of side-length a and the pyramid is assumed to be regular, i.e. its apex F is located on the orthogonal at the center E of the square at a distance h = |EF| from it (See Figure 1). The exercise asks for the determination of the height h if we know that there is a section GHIJK of the pyramid by a plane which is a regular pentagon. The section is tacitly assumed to be symmetric with respect to the diagonal symmetry plane AF C of the pyramid and defined by a plane through the three points K, G, I. The first two, K and G, lying symmetric with respect to the diagonal AC of the square.